Physics – Condensed Matter – Strongly Correlated Electrons
Scientific paper
2006-12-14
Phys.Rev.B75:214405,2007
Physics
Condensed Matter
Strongly Correlated Electrons
25 pages, 7 figures
Scientific paper
10.1103/PhysRevB.75.214405
In contrast to hole-doped systems which have hole pockets centered at $(\pm \frac{\pi}{2a},\pm \frac{\pi}{2a})$, in lightly electron-doped antiferromagnets the charged quasiparticles reside in momentum space pockets centered at $(\frac{\pi}{a},0)$ or $(0,\frac{\pi}{a})$. This has important consequences for the corresponding low-energy effective field theory of magnons and electrons which is constructed in this paper. In particular, in contrast to the hole-doped case, the magnon-mediated forces between two electrons depend on the total momentum $\vec P$ of the pair. For $\vec P = 0$ the one-magnon exchange potential between two electrons at distance $r$ is proportional to $1/r^4$, while in the hole case it has a $1/r^2$ dependence. The effective theory predicts that spiral phases are absent in electron-doped antiferromagnets.
Brügger C.
Hofmann Christoph P.
Kämpfer F.
Moser Michael
Pepe Michele
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